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CN112199818B - A method for calculating armature magnetomotive force of permanent magnet motor using star-delta connection - Google Patents

A method for calculating armature magnetomotive force of permanent magnet motor using star-delta connection Download PDF

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CN112199818B
CN112199818B CN202010908728.XA CN202010908728A CN112199818B CN 112199818 B CN112199818 B CN 112199818B CN 202010908728 A CN202010908728 A CN 202010908728A CN 112199818 B CN112199818 B CN 112199818B
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陈浈斐
汤俊
马宏忠
刘宝稳
李迅
章黄勇
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Abstract

The invention discloses an armature magnetomotive force calculation method of a permanent magnet motor adopting a star-delta connection method, which relates to the field of armature magnetomotive force calculation of fractional slot permanent magnet motors and comprises the following steps: dividing the single-phase armature winding into a star-shaped part winding and a triangular part winding; the calculating step comprises: the calculation parts comprise calculation parts such as star-shaped part winding magnetomotive force calculation, triangle-shaped part winding magnetomotive force calculation, single-phase forward synthetic magnetomotive force calculation, single-phase reverse synthetic magnetomotive force calculation and the like. The calculation method is provided for solving the problem that the armature magnetomotive force of the multilayer winding fractional slot permanent magnet motor adopting the star-delta connection method is difficult to calculate under any number of turns and mechanical angle difference, and the calculation problem of the armature magnetomotive force of the multilayer winding armature adopting the star-delta connection method is solved. The method can accurately calculate the armature magnetomotive force of the multi-layer winding fractional slot permanent magnet motor adopting the star-delta connection method, provides an effective armature magnetomotive force calculation method for the permanent magnet motor, and can be further used for other analyses of the permanent magnet motor.

Description

一种采用星-三角接法永磁电机的电枢磁动势计算方法A method for calculating armature magnetomotive force of permanent magnet motor using star-delta connection

技术领域technical field

本发明涉及分数槽永磁电机领域,特别是一种采用星-三角接法永磁电机的电枢磁动势计算方法。The invention relates to the field of fractional slot permanent magnet motors, in particular to a method for calculating armature magnetomotive force of permanent magnet motors using star-delta connection.

背景技术Background technique

相比于传统整数槽永磁电机,分数槽永磁电机转矩大、功率密度高、体积小、效率利用率高,在电动汽车、风力发电、航空航天等领域得到了广泛的应用。由于分数槽永磁电机中绕组中的电流分布,使得电枢磁动势中含有高幅值低次谐波,这些谐波在铁心、永磁体内异步运行,导致铁心和永磁体产生涡流损耗、电机产生噪声和振动等影响,使得永磁电机运行效率降低。甚至可能造成永磁体过热产生不可逆退磁、永磁电机运行异常,在使用过程中形成安全隐患。Compared with traditional integer-slot permanent magnet motors, fractional-slot permanent magnet motors have large torque, high power density, small size, and high efficiency and utilization rate, and have been widely used in electric vehicles, wind power generation, aerospace and other fields. Due to the current distribution in the windings of the fractional-slot permanent magnet motor, the armature magnetomotive force contains high-amplitude low-order harmonics. These harmonics run asynchronously in the iron core and permanent magnet, resulting in eddy current losses in the iron core and permanent magnet. The motor produces effects such as noise and vibration, which reduces the operating efficiency of the permanent magnet motor. It may even cause the permanent magnet to overheat and cause irreversible demagnetization and abnormal operation of the permanent magnet motor, which may cause potential safety hazards during use.

为了解决上述问题,国内外学者展开了广泛的研究。目前,学者们已有许多研究针对如何消除分数槽集中绕组永磁电机存在高幅值低次谐波。如研究了绕组电流相位偏移,通入多个三相电流,使其在空间和时间上选择适当的相移来减少或消除电枢磁动势谐波。通过使用每侧线圈匝数不同的线圈和在定子铁心的特定位置使用磁通屏障、不对称匝数和跨两齿距绕组结构,但是这种方法导致了输出转矩的降低。分数槽永磁电机绕组采用星-三角接法以其制造工艺简单、易于实现,受到了广大学者的关注。该方法仅通过改变分数槽永磁电机定子绕组的接法,实践表明,这种新的绕组连接方式对消除电枢磁动势谐波是非常有效的。然而,无论是星-三角接法绕组电枢磁动势谐波计算,还是多层绕组的偏移角度分析都没有系统的研究,因此在研究如何优化绕组参数以便更好地降低电枢磁动势谐波方面尚存在不足。In order to solve the above problems, scholars at home and abroad have carried out extensive research. At present, scholars have done many researches on how to eliminate the high-amplitude low-order harmonics in fractional-slot concentrated-winding permanent magnet motors. For example, the phase shift of the winding current is studied, and multiple three-phase currents are introduced to make it select the appropriate phase shift in space and time to reduce or eliminate the harmonics of the armature magnetomotive force. By using coils with a different number of turns on each side and using flux barriers at specific locations in the stator core, asymmetrical turns and a winding structure across two pitches, this approach results in a reduction in output torque. The fractional slot permanent magnet motor winding adopts the star-delta connection method, which has attracted the attention of scholars because of its simple manufacturing process and easy implementation. This method only changes the connection of the stator windings of the fractional-slot permanent magnet motor. Practice shows that this new winding connection is very effective in eliminating the harmonics of the armature magnetomotive force. However, neither the calculation of the armature magnetomotive force harmonics of the star-delta winding nor the analysis of the offset angle of the multi-layer winding has been systematically studied, so how to optimize the winding parameters to better reduce the armature magnetomotive force There are still deficiencies in potential harmonics.

发明内容SUMMARY OF THE INVENTION

本发明所要解决的技术问题是克服现有技术的不足而提供一种采用星-三角接法永磁电机的电枢磁动势计算方法,本发明通过改变电枢绕组的连接方式,对于采用给定的匝数比、相差的机械角度的定子绕组分数槽永磁电机,可以抑制电枢磁动势中低次谐波,进而抑制铁心和永磁体中涡流损耗,避免由于永磁体过热导致的不可逆退磁现象,提高永磁电机使用效率,增加电机使用的安全性。The technical problem to be solved by the present invention is to overcome the deficiencies of the prior art and provide a method for calculating armature magnetomotive force using a star-delta connection permanent magnet motor. The stator winding fractional slot permanent magnet motor with a fixed turns ratio and a different mechanical angle can suppress the low-order harmonics of the armature magnetomotive force, thereby suppressing the eddy current loss in the iron core and the permanent magnet, and avoiding the irreversible damage caused by the overheating of the permanent magnet. Demagnetization phenomenon, improve the efficiency of permanent magnet motor, increase the safety of motor use.

本发明为解决上述技术问题采用以下技术方案:The present invention adopts the following technical solutions for solving the above-mentioned technical problems:

根据本发明提出的一种采用星-三角接法永磁电机的电枢磁动势计算方法,包括以下步骤:A method for calculating armature magnetomotive force of a permanent magnet motor with star-delta connection proposed according to the present invention includes the following steps:

步骤1、对采用星-三角接法的多层绕组分数槽永磁电机,将每相电枢绕组分成星形部分绕组和三角形部分绕组;Step 1. For the multi-layer winding fractional slot permanent magnet motor using the star-delta connection method, the armature winding of each phase is divided into a star part winding and a delta part winding;

步骤2、取单相电枢绕组总匝数为Ns=NY+NΔ,NY、NΔ分别为星形部分绕组和三角形部分绕组匝数,星形部分绕组和三角形部分绕组比例系数NY'、NΔ'分别为:Step 2. Take the total number of turns of the single-phase armature winding as N s =N Y +N Δ , where N Y and N Δ are the number of turns of the star partial winding and the delta partial winding, respectively, and the proportional coefficient of the star partial winding and the delta partial winding N Y ', N Δ ' are respectively:

Figure BDA0002662447330000021
Figure BDA0002662447330000021

步骤3、根据基尔霍夫电流定律,第i相星形部分电流IiY与第i相三角形部分电流I关系为:Step 3. According to Kirchhoff's current law, the relationship between the current I iY of the ith phase star part and the current I of the ith phase triangle part is:

Figure BDA0002662447330000022
Figure BDA0002662447330000022

式中,m为永磁电机相数,i为具体相数,i=1,2,3…,星形部分绕组电流相位超前于同相的三角形部分绕组电流的相位π/2m电角度;In the formula, m is the phase number of the permanent magnet motor, i is the specific phase number, i=1, 2, 3..., the phase of the winding current of the star part is ahead of the phase π/2m electrical angle of the current of the winding current of the delta part of the same phase;

步骤4、结合星-三角接法中电枢绕组电流的相位、幅值关系,对星形部分绕组和三角形部分绕组的方波磁动势进行傅里叶分解,得到m相分数槽永磁电机星形部分绕组的电枢磁动势FYv-m为:Step 4. Combine the phase and amplitude relationship of the armature winding current in the star-delta connection method, and perform Fourier decomposition on the square wave magnetomotive force of the star partial winding and the delta partial winding to obtain an m-phase fractional slot permanent magnet motor The armature magnetomotive force F Yv-m of the star part winding is:

Figure BDA0002662447330000023
Figure BDA0002662447330000023

三角形部分绕组电枢磁动势FΔv-m为:The delta partial winding armature magnetomotive force F Δv-m is:

Figure BDA0002662447330000024
Figure BDA0002662447330000024

式中,v为电枢磁动势谐波次数,t为时间,ω为电流的角频率、I为正弦电流的有效值,Z0为单元电机定子槽数,kNvYl为永磁电机定子绕组为l层时星形部分谐波绕组系数,kNvΔl为永磁电机定子绕组为l层时三角形部分谐波绕组系数,α为永磁电机的机械角度,αs为星形部分绕组和三角形部分绕组相差机械角度;In the formula, v is the armature magnetomotive force harmonic order, t is the time, ω is the angular frequency of the current, I is the effective value of the sinusoidal current, Z 0 is the number of stator slots of the unit motor, and k NvYl is the permanent magnet motor stator winding is the star-shaped partial harmonic winding coefficient when the layer is l, k NvΔl is the triangular partial harmonic winding coefficient when the stator winding of the permanent magnet motor is l-layer, α is the mechanical angle of the permanent magnet motor, α s is the star-shaped partial winding and the triangular part Winding difference mechanical angle;

步骤5、若星形部分绕组和三角形部分绕组电枢磁动势相量方向相同,对星形部分绕组和三角形部分绕组电枢磁动势合成,得到单相正向合成电枢磁动势Ftv-m为:Step 5. If the phasors of the armature magnetomotive force of the star part winding and the delta part winding are in the same direction, synthesize the armature magnetomotive force of the star part winding and the delta part winding to obtain the single-phase forward synthetic armature magnetomotive force F tv-m is:

Figure BDA0002662447330000025
Figure BDA0002662447330000025

其中,ht-YΔm为m相永磁电机中星-三角形部分绕组电枢磁动势正向合成因数,

Figure BDA0002662447330000026
为m相永磁电机三角形部分绕组电枢磁动势偏移角度;Among them, h t-YΔm is the forward synthesis factor of the armature magnetomotive force of the star-delta part winding in the m-phase permanent magnet motor,
Figure BDA0002662447330000026
is the armature magnetomotive force offset angle of the triangular part winding of the m-phase permanent magnet motor;

步骤6、若星形部分绕组和三角形部分绕组电枢磁动势相量方向相反,得到单相反向合成磁动势Ftv-m'为:Step 6. If the armature magnetomotive force phasors of the star-shaped partial winding and the delta partial winding are in opposite directions, the single-phase reverse synthetic magnetomotive force F tv-m ' is obtained as:

Figure BDA0002662447330000031
Figure BDA0002662447330000031

式中,ht-YΔm'为m相永磁电机中星-三角形部分绕组电枢磁动势反向合成因数。In the formula, h t-YΔm ' is the reverse synthesis factor of the armature magnetomotive force of the star-delta partial winding in the m-phase permanent magnet motor.

作为本发明所述的一种采用星-三角接法永磁电机的电枢磁动势计算方法进一步优化方案,

Figure BDA0002662447330000032
As a further optimization scheme of the armature magnetomotive force calculation method of the star-delta connection permanent magnet motor according to the present invention,
Figure BDA0002662447330000032

作为本发明所述的一种采用星-三角接法永磁电机的电枢磁动势计算方法进一步优化方案,

Figure BDA0002662447330000033
As a further optimization scheme of the armature magnetomotive force calculation method of the star-delta connection permanent magnet motor according to the present invention,
Figure BDA0002662447330000033

作为本发明所述的一种采用星-三角接法永磁电机的电枢磁动势计算方法进一步优化方案,

Figure BDA0002662447330000034
As a further optimization scheme of the armature magnetomotive force calculation method of the star-delta connection permanent magnet motor according to the present invention,
Figure BDA0002662447330000034

作为本发明所述的一种采用星-三角接法永磁电机的电枢磁动势计算方法进一步优化方案,对于采用给定绕组匝数比、机械角度差的星形部分绕组和三角形部分绕组的分数槽永磁电机,单相反向合成磁动势Ftv-m'的步骤具体如下:As a further optimization scheme of the armature magnetomotive force calculation method of the permanent magnet motor using the star-delta connection method of the present invention, for the star partial winding and the delta partial winding with a given winding turns ratio and mechanical angle difference For the fractional slot permanent magnet motor, the steps of unidirectionally synthesizing the magnetomotive force F tv-m ' are as follows:

步骤(1)、保持星形部分绕组和三角形部分绕组均匀分布在每相不同的扇区中,即星形部分谐波绕组系数与三角形部分谐波绕组系数相同;Step (1), keep the star partial winding and the delta partial winding evenly distributed in different sectors of each phase, that is, the star partial harmonic winding coefficient is the same as the delta partial harmonic winding coefficient;

kNvYl=kNvΔlk NvYl =k NvΔl ;

其中,l=2k,k=1,2,3…,l为永磁电机绕组层数,kNvYl为永磁电机定子绕组为l层时星形部分谐波绕组系数,kNvΔl为永磁电机定子绕组为l层时三角形部分谐波绕组系数;Among them, l=2k, k=1, 2, 3..., l is the number of PM motor winding layers, k NvYl is the star-shaped partial harmonic winding coefficient when the permanent magnet motor stator winding is l-layer, and k NvΔl is the PM motor When the stator winding is l-layer, the triangular partial harmonic winding coefficient;

步骤(2)、保持星形部分绕组和三角形部分绕组磁动势幅值一致,仅考虑星形部分绕组和三角形部分绕组电枢磁动势相量方向相反的情况;Step (2), keep the magnetomotive force amplitudes of the star part winding and the delta part winding consistent, and only consider the situation where the armature magnetomotive force phasor directions of the star part winding and the delta part winding are opposite;

Figure BDA0002662447330000035
Figure BDA0002662447330000035

式中,

Figure BDA0002662447330000036
为星形部分绕组电流,
Figure BDA0002662447330000037
为三角形部分绕组电流;In the formula,
Figure BDA0002662447330000036
is the winding current of the star part,
Figure BDA0002662447330000037
is the winding current of the delta part;

步骤(3)、对于m相四层绕组分数槽永磁电机,采用第一扇区为星形部分绕组,第二扇区为三角形部分绕组;星形部分绕组和三角形部分绕组中电流的相位差为π/2m,星-三角部分绕组相差的机械角度由第二个扇区偏移角度αp所决定Step (3), for the m-phase four-layer winding fractional slot permanent magnet motor, the first sector is a star partial winding, and the second sector is a delta partial winding; the phase difference of the current in the star partial winding and the delta partial winding is used is π/2m, the mechanical angle of the star-delta winding phase difference is determined by the offset angle α p of the second sector

Figure BDA0002662447330000041
Figure BDA0002662447330000041

式中,α0为分数槽永磁电机的槽距角;In the formula, α 0 is the slot pitch angle of the fractional slot permanent magnet motor;

步骤(4)、当m相四层绕组分数槽永磁电机中单元电机定子槽数为Z0=4mk时,能够抑制低次电枢磁动势,则单相反向合成磁动势Ftv-m'为:Step (4), when the number of stator slots of the unit motor in the m-phase four-layer winding fractional slot permanent magnet motor is Z 0 =4mk, the low-order armature magnetomotive force can be suppressed, and the single-phase reverse synthetic magnetomotive force F tv- m ' is:

Figure BDA0002662447330000042
Figure BDA0002662447330000042

其中,kNvY4为永磁电机绕组为四层时的星形部分、三角形部分的谐波绕组系数。Among them, k NvY4 is the harmonic winding coefficient of the star part and the triangle part when the permanent magnet motor winding is four layers.

本发明采用以上技术方案与现有技术相比,具有以下技术效果:Compared with the prior art, the present invention adopts the above technical scheme, and has the following technical effects:

本发明提出的计算方法解决了定子层数偶数的任意m相分数槽永磁电机对任意匝数、相差机械角度电枢磁动势计算问题;通过改变电枢绕组的连接方式,对于采用给定的匝数比、相差的机械角度的定子绕组分数槽永磁电机,可以抑制电枢磁动势中低次谐波,进而抑制铁心和永磁体中涡流损耗,避免由于永磁体过热导致的不可逆退磁现象,提高永磁电机使用效率,增加电机使用的安全性。The calculation method proposed by the invention solves the calculation problem of the armature magnetomotive force of any m-phase fractional slot permanent magnet motor with an even number of stator layers for any number of turns and a mechanical angle difference; The stator winding fractional slot permanent magnet motor with the highest turns ratio and different mechanical angles can suppress the low-order harmonics of the armature magnetomotive force, thereby suppressing the eddy current loss in the iron core and the permanent magnet, and avoiding the irreversible demagnetization caused by the overheating of the permanent magnet. phenomenon, improve the efficiency of permanent magnet motor use, and increase the safety of motor use.

附图说明Description of drawings

图1为本发明所描述的采用星-三角接法的多层绕组分数槽永磁电机绕组接法示意图。FIG. 1 is a schematic diagram of the winding connection method of the multi-layer winding fractional slot permanent magnet motor using the star-delta connection method described in the present invention.

图2为图1中采用星-三角接法的分数槽永磁电机绕组中电流相位、幅值示意图。FIG. 2 is a schematic diagram of the current phase and amplitude in the winding of the fractional slot permanent magnet motor using the star-delta connection method in FIG. 1 .

图3为图1中采用星-三角接法的分数槽永磁电机绕组中电枢磁动势示意图;其中,(a)为k=1时电枢磁动势,(b)为k=3时电枢磁动势。Figure 3 is a schematic diagram of the armature magnetomotive force in the winding of the fractional slot permanent magnet motor using the star-delta connection method in Figure 1; wherein, (a) is the armature magnetomotive force when k=1, (b) is k=3 When the armature magnetomotive force.

图4为四种不同绕组结构的分数槽永磁电机示意图;其中,(a)为Y-Y接法双层绕组永磁电机,(b)为Y-Δ接法双层绕组永磁电机,(c)为Y-Y接法四层绕组永磁电机,(d)为Y-Δ接法双层绕组永磁电机。Figure 4 is a schematic diagram of a fractional-slot permanent magnet motor with four different winding structures; among them, (a) is a Y-Y connection double-winding permanent magnet motor, (b) is a Y-Δ connection double-winding permanent magnet motor, (c) ) is a four-layer winding permanent magnet motor with Y-Y connection, and (d) is a double-winding permanent magnet motor with Y-Δ connection.

图5为图4中不同绕组结构的分数槽永磁电机的电枢磁动势示意图;其中,(a)为Y-Y接法双层绕组永磁电机电枢磁动势,(b)为Y-Δ接法双层绕组永磁电机电枢磁动势,(c)为Y-Y接法四层绕组永磁电机电枢磁动势,(d)为Y-Δ接法四层绕组永磁电机电枢磁动势。Figure 5 is a schematic diagram of the armature magnetomotive force of the fractional slot permanent magnet motor with different winding structures in Figure 4; wherein, (a) is the armature magnetomotive force of the Y-Y connection double-layer winding permanent magnet motor, and (b) is the Y- The armature magnetomotive force of the double-layer winding permanent magnet motor with Δ connection method, (c) is the armature magnetomotive force of the four-layer winding permanent magnet motor with Y-Y connection method, and (d) is the magnetomotive force of the four-layer winding permanent magnet motor with Y-Δ connection method. Pivot magnetomotive force.

具体实施方式Detailed ways

下面结合附图对本发明的技术方案做进一步的详细说明:Below in conjunction with accompanying drawing, the technical scheme of the present invention is described in further detail:

本发明所描述的实施例仅是针对采用星-三角接法多层绕的分数槽永磁电机,而本发明也可应用到采用星-三角接法其他任意匝数比、偏移角度多层绕组的分数槽永磁电机中。The embodiment described in the present invention is only for the fractional slot permanent magnet motor with multi-layer winding in star-delta connection, and the present invention can also be applied to other arbitrary turns ratio and offset angle multi-layered motor in star-delta connection. Windings in fractional slot permanent magnet motors.

实施例1Example 1

对采用星-三角接法的多层绕组的m相分数槽永磁电机,将每相电枢绕组分成星形部分电枢绕组和三角形部分电枢绕组,如图1所示。For the m-phase fractional slot permanent magnet motor with multi-layer windings in star-delta connection, the armature windings of each phase are divided into star-shaped partial armature windings and delta-shaped partial armature windings, as shown in Figure 1.

为了简便计算,取单相电枢绕组总匝数为Ns=NY+NΔ,星形部分绕组和三角形部分绕组比例系数为:In order to simplify the calculation, the total number of turns of the single-phase armature winding is taken as N s =N Y +N Δ , and the proportional coefficient of the star part winding and the delta part winding is:

Figure BDA0002662447330000051
Figure BDA0002662447330000051

根据基尔霍夫电流定律,星形部分绕组电流IiY与三角部分绕组电流I关系为:

Figure BDA0002662447330000052
According to Kirchhoff's current law, the relationship between the star winding current I iY and the delta winding current I is:
Figure BDA0002662447330000052

式中,i为具体相数(i=1,2,3…),星形部分绕组电流相位超前于同相的三角形部分绕组电流的相位π/2m电角度,具体电流相位、幅值关系如图2所示。In the formula, i is the specific phase number (i=1, 2, 3...), the phase of the star winding current is ahead of the phase π/2m electrical angle of the in-phase delta winding current, and the specific current phase and amplitude relationship is shown in the figure 2 shown.

对星形部分绕组和三角形部分绕组方波磁动势通过傅里叶分解,可得星形部分绕组电枢磁动势为:The square wave magnetomotive force of the star partial winding and the delta partial winding is decomposed by Fourier, and the armature magnetomotive force of the star partial winding can be obtained as:

Figure BDA0002662447330000053
Figure BDA0002662447330000053

三角形部分绕组电枢磁动势为:The armature magnetomotive force of the delta winding is:

Figure BDA0002662447330000054
Figure BDA0002662447330000054

式中,v为电枢磁动势谐波次数,t为时间,ω为电流的角频率、I为正弦电流的有效值,Z0为单元电机定子槽数,kNvYl为永磁电机定子绕组为l层时星形部分谐波绕组系数,kNvΔl为永磁电机定子绕组为l层时三角形部分谐波绕组系数,α为永磁电机的机械角度,αs为星形部分绕组和三角形部分绕组相差机械角度;In the formula, v is the armature magnetomotive force harmonic order, t is the time, ω is the angular frequency of the current, I is the effective value of the sinusoidal current, Z 0 is the number of stator slots of the unit motor, and k NvYl is the permanent magnet motor stator winding is the star-shaped partial harmonic winding coefficient when the layer is l, k NvΔl is the triangular partial harmonic winding coefficient when the stator winding of the permanent magnet motor is l-layer, α is the mechanical angle of the permanent magnet motor, α s is the star-shaped partial winding and the triangular part Winding difference mechanical angle;

若星形部分绕组和三角形部分绕组电枢磁动势相量方向相同,对星形部分绕组和三角形部分绕组电枢磁动势合成,可得单相正向合成电枢磁动势为:If the phasors of the armature magnetomotive force of the star part winding and the delta part winding are in the same direction, and the armature magnetomotive force of the star part winding and the delta part winding are synthesized, the single-phase forward combined armature magnetomotive force can be obtained as:

Figure BDA0002662447330000055
Figure BDA0002662447330000055

式中,ht-YΔm为m相永磁电机中星-三角形部分绕组电枢磁动势正向合成因数In the formula, h t-YΔm is the forward synthesis factor of the armature magnetomotive force of the star-delta partial winding in the m-phase permanent magnet motor

Figure BDA0002662447330000061
Figure BDA0002662447330000061

其中,

Figure BDA0002662447330000067
为m相永磁电机三角形部分绕组电枢磁动势偏移角度in,
Figure BDA0002662447330000067
is the offset angle of the armature magnetomotive force of the delta winding of the m-phase permanent magnet motor

Figure BDA0002662447330000062
Figure BDA0002662447330000062

若星形部分绕组和三角形部分绕组电枢磁动势相量方向相反,可得单相反向合成磁动势为:If the phasors of the armature magnetomotive force of the star part winding and the delta part winding are opposite in direction, the single-phase reverse combined magnetomotive force can be obtained as:

Figure BDA0002662447330000063
Figure BDA0002662447330000063

式中,ht-YΔm'为m相永磁电机中星-三角形部分绕组电枢磁动势反向合成因数In the formula, h t-YΔm ' is the reverse synthesis factor of the armature magnetomotive force of the star-delta partial winding in the m-phase permanent magnet motor

Figure BDA0002662447330000064
Figure BDA0002662447330000064

在给定的星形部分绕组和三角形部分绕组的匝数比、相差机械角度对于抑制低次磁动势谐波分量步骤具体为:The steps for suppressing the harmonic components of low-order magnetomotive force at a given turn ratio and mechanical angle of the star-shaped partial winding and the delta-shaped partial winding are as follows:

保持星形部分绕组和三角形部分绕组均匀分布在每相不同的扇区中,即星形部分谐波绕组系数与三角形部分谐波绕组系数相同Keep the star partial winding and the delta partial winding evenly distributed in different sectors of each phase, that is, the star partial harmonic winding coefficient is the same as the delta partial harmonic winding coefficient

kNvYl=kNvΔl k NvYl =k NvΔl

其中,l=2k,k=1,2,3…,l为永磁电机绕组层数,kNvYl为永磁电机定子绕组为l层时星形部分谐波绕组系数,kNvΔl为永磁电机定子绕组为l层时三角形部分谐波绕组系数;Among them, l=2k, k=1, 2, 3..., l is the number of PM motor winding layers, k NvYl is the star-shaped partial harmonic winding coefficient when the permanent magnet motor stator winding is l-layer, and k NvΔl is the PM motor When the stator winding is l-layer, the triangular partial harmonic winding coefficient;

保持星形部分绕组和三角形部分绕组磁动势幅值一致,仅考虑星形部分绕组和三角形部分绕组电枢磁动势相量方向相反的情况Keep the magnetomotive force amplitudes of the star partial winding and the delta partial winding consistent, and only consider the situation where the armature magnetomotive force phasors of the star partial winding and the delta partial winding are in opposite directions

Figure BDA0002662447330000065
Figure BDA0002662447330000065

对于m相四层绕组分数槽永磁电机,采用第一扇区为星形部分绕组,第二扇区为三角形绕组。星形部分绕组和三角形部分绕组中电流的相位差为π/2m,星-三角部分绕组相差的机械角度由第二个扇区偏移角度αp所决定For the m-phase four-layer winding fractional slot permanent magnet motor, the first sector is a star partial winding, and the second sector is a delta winding. The phase difference of the current in the star partial winding and the delta partial winding is π/2m, and the mechanical angle of the star-delta partial winding difference is determined by the second sector offset angle α p

Figure BDA0002662447330000066
Figure BDA0002662447330000066

当m相四层绕组分数槽永磁电机中单元电机定子槽数为Z0=4mk时,可抑制低次电枢磁动势,不同定子槽数的分数槽永磁电机电枢磁动势如图3所示,其中,图3中的(a)为k=1时电枢磁动势,图3中的(b)为k=3时电枢磁动势;单相电枢磁动势为When the number of stator slots of the unit motor in the m-phase four-layer winding fractional-slot permanent magnet motor is Z 0 =4mk, the low-order armature magnetomotive force can be suppressed. The armature magnetomotive force of the fractional slot permanent magnet motor with different stator slots is as follows As shown in Figure 3, (a) in Figure 3 is the armature magnetomotive force when k=1, and (b) in Figure 3 is the armature magnetomotive force when k=3; single-phase armature magnetomotive force for

Figure BDA0002662447330000071
Figure BDA0002662447330000071

其中,kNvY4为永磁电机绕组为四层时的星形部分、三角形部分的谐波绕组系数。Among them, k NvY4 is the harmonic winding coefficient of the star part and the triangle part when the permanent magnet motor winding is four layers.

本实施例中,为了对比采用给定的星-三角接法的分数槽永磁电机对于低次电枢磁动势谐波的抑制效果,将对采用星-星接法、星-三角接法的不同绕组层数的10极12槽分数槽永磁电机电枢磁动势进行仿真。假设所有设计的转子尺寸、永磁体大小、充磁方式、排列方式、铜体积均一致的情况下,图4为四台不同绕组结构的分数槽永磁电机,图4中的(a)为Y-Y接法双层绕组永磁电机,图4中的(b)为Y-Δ接法双层绕组永磁电机,图4中的(c)为Y-Y接法四层绕组永磁电机,图4中的(d)为Y-Δ接法双层绕组永磁电机。四种不同绕组结构的分数槽永磁电机定子槽数Z为12,转子极对数p为5,表1为四种分数槽永磁电机中相同的基本参数。In this embodiment, in order to compare the suppression effect of the fractional slot permanent magnet motor with a given star-delta connection on the harmonics of the low-order armature magnetomotive force, the star-star connection and the star-delta connection will be used. The armature magnetomotive force of the 10-pole 12-slot fractional-slot permanent magnet motor with different winding layers is simulated. Assuming that all designed rotor sizes, permanent magnet sizes, magnetization methods, arrangement methods, and copper volumes are the same, Figure 4 shows four fractional-slot permanent magnet motors with different winding structures, and (a) in Figure 4 is Y-Y Connection double-layer winding permanent magnet motor, (b) in Figure 4 is a Y-Δ connection double-layer winding permanent magnet motor, Figure 4 (c) is a Y-Y connection four-layer winding permanent magnet motor, in Figure 4 (d) is a Y-Δ connection double-winding permanent magnet motor. The fractional slot permanent magnet motor with four different winding structures has a stator slot number Z of 12 and a rotor pole pair number p of 5. Table 1 shows the same basic parameters of the four fractional slot permanent magnet motors.

表1Table 1

Figure BDA0002662447330000072
Figure BDA0002662447330000072

若三相多层绕组分数槽永磁电机的单元电机定子槽数为12时,则分数槽永磁电机的单相电枢磁动势为:If the number of stator slots of the unit motor of the three-phase multi-layer winding fractional-slot permanent magnet motor is 12, the single-phase armature magnetomotive force of the fractional-slot permanent magnet motor is:

Figure BDA0002662447330000073
Figure BDA0002662447330000073

在本实施例中,四种不同绕组结构的分数槽永磁电机对应电枢磁动势如图5所示,图5中的(a)为Y-Y接法双层绕组永磁电机电枢磁动势,图5中的(b)为Y-Δ接法双层绕组永磁电机电枢磁动势,图5中的(c)为Y-Y接法四层绕组永磁电机电枢磁动势,图5中的(d)为Y-Δ接法四层绕组永磁电机电枢磁动势。对所得不同绕组结构的电枢磁动势进行傅里叶分解,可得各次数的谐波幅值如表2所示。In this embodiment, the corresponding armature magnetomotive force of the fractional-slot permanent magnet motor with four different winding structures is shown in Figure 5, and (a) in Figure 5 is the armature magnetomotive force of the Y-Y connection double-layer winding permanent magnet motor. (b) in Figure 5 is the armature magnetomotive force of the Y-Δ connection double-layer winding permanent magnet motor, and (c) in Figure 5 is the armature magnetomotive force of the four-layer winding permanent magnet motor with Y-Y connection, (d) in Fig. 5 is the magnetomotive force of the armature of the four-layer winding permanent magnet motor with Y-Δ connection. Perform Fourier decomposition on the armature magnetomotive force of the obtained different winding structures, and the harmonic amplitudes of each order can be obtained as shown in Table 2.

表2实施例一中不同绕组结构各谐波次数的幅值百分比Table 2 Amplitude percentage of each harmonic order of different winding structures in Example 1

Figure BDA0002662447330000081
Figure BDA0002662447330000081

对应表2可知,采用星-三角接法多层绕组三相永磁电机可以完全消除谐波次数为v=1,11,13,23,26…等次数的电枢谐波磁动势,证明了分数槽永磁电机绕组采用星-三角接法通过抑制低次谐波,可以有效降低永磁电机定、转子的铁心损耗和永磁体的涡流损耗,提高永磁电机使用效率,增加电机使用的安全性。Corresponding to Table 2, it can be seen that the multi-layer winding three-phase permanent magnet motor with star-delta connection can completely eliminate the armature harmonic magnetomotive force with harmonic orders of v=1, 11, 13, 23, 26, etc. It is proved that The fractional slot permanent magnet motor winding adopts the star-delta connection method to suppress the low-order harmonics, which can effectively reduce the iron core loss of the permanent magnet motor and the rotor and the eddy current loss of the permanent magnet, improve the use efficiency of the permanent magnet motor, and increase the use of the motor. safety.

这里以本发明的实施例为中心,详细介绍了本方法的具体计算过程。所描述的计算流程或某些特征的具体体现,应当理解为本说明书仅仅是针对给出实施例的电机结构来描述本发明,实际上对于不同绕组结构的分数槽永磁电机电枢磁动势分析时某些细节上会有所变化,这些变化应该属于本发明范围内。Centering on the embodiments of the present invention, the specific calculation process of the method is described in detail here. The described calculation process or the specific embodiment of some features should be understood that this specification is only for describing the present invention with respect to the motor structure of the given embodiment. In fact, for fractional slot permanent magnet motor armature magnetomotive force of different winding structures Certain details may vary during the analysis, and these variations should fall within the scope of the present invention.

本领域技术人员可以理解附图只是一个优选实施例的示意图,上述本发明实施例仅仅为了描述,不代表实施例的优劣。以上所述仅为本发明的较佳实施例,并不用以限制本发明,凡在本发明的精神和原则之内,所作的任何修改、等同替换、改进等,均应包含在本发明的保护范围之内。Those skilled in the art can understand that the accompanying drawing is only a schematic diagram of a preferred embodiment, and the above embodiments of the present invention are only for description, and do not represent the advantages or disadvantages of the embodiments. The above are only preferred embodiments of the present invention and are not intended to limit the present invention. Any modifications, equivalent replacements, improvements, etc. made within the spirit and principles of the present invention shall be included in the protection of the present invention. within the range.

Claims (5)

1.一种采用星-三角接法永磁电机的电枢磁动势计算方法,其特征在于,包括以下步骤:1. a method for calculating armature magnetomotive force using star-delta connection permanent magnet motor, is characterized in that, comprises the following steps: 步骤1、对采用星-三角接法的多层绕组分数槽永磁电机,将每相电枢绕组分成星形部分绕组和三角形部分绕组;Step 1. For the multi-layer winding fractional slot permanent magnet motor using the star-delta connection method, the armature winding of each phase is divided into a star part winding and a delta part winding; 步骤2、取单相电枢绕组总匝数为Ns=NY+NΔ,NY、NΔ分别为星形部分绕组和三角形部分绕组匝数,星形部分绕组和三角形部分绕组比例系数NY'、NΔ'分别为:Step 2. Take the total number of turns of the single-phase armature winding as N s =N Y +N Δ , where N Y and N Δ are the number of turns of the star partial winding and the delta partial winding, respectively, and the proportional coefficient of the star partial winding and the delta partial winding N Y ', N Δ ' are respectively:
Figure FDA0002662447320000011
Figure FDA0002662447320000011
步骤3、根据基尔霍夫电流定律,第i相星形部分电流IiY与第i相三角形部分电流I关系为:Step 3. According to Kirchhoff's current law, the relationship between the current I iY of the ith phase star part and the current I of the ith phase triangle part is:
Figure FDA0002662447320000012
Figure FDA0002662447320000012
式中,m为永磁电机相数,i为具体相数,i=1,2,3…,星形部分绕组电流相位超前于同相的三角形部分绕组电流的相位π/2m电角度;In the formula, m is the phase number of the permanent magnet motor, i is the specific phase number, i=1, 2, 3..., the phase of the winding current of the star part is ahead of the phase π/2m electrical angle of the current of the winding current of the delta part of the same phase; 步骤4、结合星-三角接法中电枢绕组电流的相位、幅值关系,对星形部分绕组和三角形部分绕组的方波磁动势进行傅里叶分解,得到m相分数槽永磁电机星形部分绕组的电枢磁动势FYv-m为:Step 4. Combine the phase and amplitude relationship of the armature winding current in the star-delta connection method, and perform Fourier decomposition on the square wave magnetomotive force of the star partial winding and the delta partial winding to obtain an m-phase fractional slot permanent magnet motor The armature magnetomotive force F Yv-m of the star part winding is:
Figure FDA0002662447320000013
Figure FDA0002662447320000013
三角形部分绕组电枢磁动势FΔv-m为:The delta partial winding armature magnetomotive force F Δv-m is:
Figure FDA0002662447320000014
Figure FDA0002662447320000014
式中,v为电枢磁动势谐波次数,t为时间,ω为电流的角频率、I为正弦电流的有效值,Z0为单元电机定子槽数,kNvYl为永磁电机定子绕组为l层时星形部分谐波绕组系数,kNvΔl为永磁电机定子绕组为l层时三角形部分谐波绕组系数,α为永磁电机的机械角度,αs为星形部分绕组和三角形部分绕组相差机械角度;In the formula, v is the armature magnetomotive force harmonic order, t is the time, ω is the angular frequency of the current, I is the effective value of the sinusoidal current, Z 0 is the number of stator slots of the unit motor, and k NvYl is the permanent magnet motor stator winding is the star-shaped partial harmonic winding coefficient when the layer is l, k NvΔl is the triangular partial harmonic winding coefficient when the stator winding of the permanent magnet motor is l-layer, α is the mechanical angle of the permanent magnet motor, α s is the star-shaped partial winding and the triangular part Winding difference mechanical angle; 步骤5、若星形部分绕组和三角形部分绕组电枢磁动势相量方向相同,对星形部分绕组和三角形部分绕组电枢磁动势合成,得到单相正向合成电枢磁动势Ftv-m为:Step 5. If the phasors of the armature magnetomotive force of the star part winding and the delta part winding are in the same direction, synthesize the armature magnetomotive force of the star part winding and the delta part winding to obtain the single-phase forward synthetic armature magnetomotive force F tv-m is:
Figure FDA0002662447320000021
Figure FDA0002662447320000021
其中,ht-YΔm为m相永磁电机中星-三角形部分绕组电枢磁动势正向合成因数,
Figure FDA0002662447320000022
为m相永磁电机三角形部分绕组电枢磁动势偏移角度;
Among them, h t-YΔm is the forward synthesis factor of the armature magnetomotive force of the star-delta part winding in the m-phase permanent magnet motor,
Figure FDA0002662447320000022
is the armature magnetomotive force offset angle of the triangular part winding of the m-phase permanent magnet motor;
步骤6、若星形部分绕组和三角形部分绕组电枢磁动势相量方向相反,得到单相反向合成磁动势Ftv-m'为:Step 6. If the armature magnetomotive force phasors of the star-shaped partial winding and the delta partial winding are in opposite directions, the single-phase reverse synthetic magnetomotive force F tv-m ' is obtained as:
Figure FDA0002662447320000023
Figure FDA0002662447320000023
式中,ht-YΔm'为m相永磁电机中星-三角形部分绕组电枢磁动势反向合成因数。In the formula, h t-YΔm ' is the reverse synthesis factor of the armature magnetomotive force of the star-delta partial winding in the m-phase permanent magnet motor.
2.根据权利要求1所述的一种采用星-三角接法永磁电机的电枢磁动势计算方法,其特征在于,
Figure FDA0002662447320000024
2. a kind of armature magnetomotive force calculation method adopting star-delta connection permanent magnet motor according to claim 1, is characterized in that,
Figure FDA0002662447320000024
3.根据权利要求1所述的一种采用星-三角接法永磁电机的电枢磁动势计算方法,其特征在于,
Figure FDA0002662447320000025
3. a kind of armature magnetomotive force calculation method adopting star-delta connection permanent magnet motor according to claim 1, is characterized in that,
Figure FDA0002662447320000025
4.根据权利要求1所述的一种采用星-三角接法永磁电机的电枢磁动势计算方法,其特征在于,
Figure FDA0002662447320000026
4. a kind of armature magnetomotive force calculation method using star-delta connection permanent magnet motor according to claim 1, is characterized in that,
Figure FDA0002662447320000026
5.根据权利要求1所述的一种采用星-三角接法永磁电机的电枢磁动势计算方法,其特征在于,对于采用给定绕组匝数比、机械角度差的星形部分绕组和三角形部分绕组的分数槽永磁电机,单相反向合成磁动势Ftv-m'的步骤具体如下:5. a kind of armature magnetomotive force calculation method adopting star-delta connection permanent magnet motor according to claim 1, is characterized in that, for adopting the star-shaped partial winding of given winding turns ratio, mechanical angle difference And the fractional-slot permanent magnet motor with delta partial winding, the steps of uniphase reverse synthesis of magnetomotive force F tv-m ' are as follows: 步骤(1)、保持星形部分绕组和三角形部分绕组均匀分布在每相不同的扇区中,即星形部分谐波绕组系数与三角形部分谐波绕组系数相同;Step (1), keep the star partial winding and the delta partial winding evenly distributed in different sectors of each phase, that is, the star partial harmonic winding coefficient is the same as the delta partial harmonic winding coefficient; kNvYl=kNvΔlk NvYl =k NvΔl ; 其中,l=2k,k=1,2,3…,l为永磁电机绕组层数,kNvYl为永磁电机定子绕组为l层时星形部分谐波绕组系数,kNvΔl为永磁电机定子绕组为l层时三角形部分谐波绕组系数;Among them, l=2k, k=1, 2, 3..., l is the number of PM motor winding layers, k NvYl is the star-shaped partial harmonic winding coefficient when the permanent magnet motor stator winding is l-layer, and k NvΔl is the PM motor When the stator winding is l-layer, the triangular partial harmonic winding coefficient; 步骤(2)、保持星形部分绕组和三角形部分绕组磁动势幅值一致,仅考虑星形部分绕组和三角形部分绕组电枢磁动势相量方向相反的情况;Step (2), keep the magnetomotive force amplitudes of the star part winding and the delta part winding consistent, and only consider the situation where the armature magnetomotive force phasor directions of the star part winding and the delta part winding are opposite;
Figure FDA0002662447320000031
Figure FDA0002662447320000031
式中,
Figure FDA0002662447320000036
为星形部分绕组电流,
Figure FDA0002662447320000033
为三角形部分绕组电流;
In the formula,
Figure FDA0002662447320000036
is the winding current of the star part,
Figure FDA0002662447320000033
is the winding current of the delta part;
步骤(3)、对于m相四层绕组分数槽永磁电机,采用第一扇区为星形部分绕组,第二扇区为三角形部分绕组;星形部分绕组和三角形部分绕组中电流的相位差为π/2m,星-三角部分绕组相差的机械角度由第二个扇区偏移角度αp所决定Step (3), for the m-phase four-layer winding fractional slot permanent magnet motor, the first sector is a star partial winding, and the second sector is a delta partial winding; the phase difference of the current in the star partial winding and the delta partial winding is used is π/2m, the mechanical angle of the star-delta winding phase difference is determined by the offset angle α p of the second sector
Figure FDA0002662447320000034
Figure FDA0002662447320000034
式中,α0为分数槽永磁电机的槽距角;In the formula, α 0 is the slot pitch angle of the fractional slot permanent magnet motor; 步骤(4)、当m相四层绕组分数槽永磁电机中单元电机定子槽数为Z0=4mk时,能够抑制低次电枢磁动势,则单相反向合成磁动势Ftv-m'为:Step (4), when the number of stator slots of the unit motor in the m-phase four-layer winding fractional slot permanent magnet motor is Z 0 =4mk, the low-order armature magnetomotive force can be suppressed, and the single-phase reverse synthetic magnetomotive force F tv- m ' is:
Figure FDA0002662447320000035
Figure FDA0002662447320000035
其中,kNvY4为永磁电机绕组为四层时的星形部分、三角形部分的谐波绕组系数。Among them, k NvY4 is the harmonic winding coefficient of the star part and the triangle part when the permanent magnet motor winding is four layers.
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